We note that the mass of the NP model, namely LQ for the present case, is theoretically restricted apart from the above bounds.
For instance, once we employ the unitarity bound for NP in \(b \rightarrow c \tau \nu \)  to explain the \(R_{D^{(*)}}\)  excesses,
the NP mass is restricted as \(\lesssim 9\,\text{TeV}\)  [1]}.
If this is the case, the EFT limit is never valid for the LHC analysis.A loose restriction is obtained from Fig. REF .
Therefore, our non-EFT study is of critical importance and useful for practical NP scenarios.
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